中国物理B ›› 2025, Vol. 34 ›› Issue (8): 86302-086302.doi: 10.1088/1674-1056/adda0e

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Lattice and phonon properties in semiconductors FeSb2 and RuSb2

Meng Zhang(张萌)1, Shengnan Dai(戴胜男)2,†, Ranran Zhang(张冉冉)3, Mingfang Shu(舒明方)1, Wei Xu(徐威)1, Jinfeng Zhu(朱金峰)1, Xianglin Liu(刘祥麟)4, Yixuan Luo(罗伊轩)4, Toru Ishigaki5, Bo Duan(段波)6, Yanfeng Guo(郭艳峰)4,7, Zhe Qu(屈哲)3, Jiong Yang(杨炯)2, and Jie Ma(马杰)1,‡   

  1. 1 Key Laboratory of Artificial Structures and Quantum Control, School of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai 200240, China;
    2 Materials Genome Institute, Shanghai University, Shanghai 200444, China;
    3 Anhui Key Laboratory of Low-Energy Quantum Materials and Devices, High Magnetic Field Laboratory, Hefei Institutes of Physical Science, Chinese Academy of Sciences, Hefei 230031, China;
    4 School of Physical Science and Technology, ShanghaiTech University, Shanghai 201210, China;
    5 Neutron Industrial Application Promotion Center, Comprehensive Research Organization for Science and Society, Naka, Ibaraki 319-1106, Japan;
    6 Hubei Key Laboratory of Theory and Application of Advanced Materials Mechanics, School of Science, Wuhan University of Technology, Wuhan 430070, China;
    7 ShanghaiTech Laboratory for Topological Physics, ShanghaiTech University, Shanghai 201210, China
  • 收稿日期:2025-04-05 修回日期:2025-05-06 接受日期:2025-05-19 出版日期:2025-07-17 发布日期:2025-08-05
  • 通讯作者: Shengnan Dai, Jie Ma E-mail:musenc@shu.edu.cn;jma3@sjtu.edu.cn
  • 基金资助:
    Project supported by the National Natural Science Foundation of China (Grant Nos. U2032213 and 12334008), the Guangdong Provincial Key Laboratory of Extreme Conditions (Grant No. 2023B1212010002). We thank the staff members of the Micro-Raman Spectroscopy System (https://cstr.cn/31125.02.SHMFF.RAMAN) at the Steady High Magnetic Field Facility, CAS (https://cstr.cn/31125.02.SHMFF), for providing technical support and assistance in data collection and analysis. We acknowledge the beam time granted by J-PARC (proposal No. 2019A0191).

Lattice and phonon properties in semiconductors FeSb2 and RuSb2

Meng Zhang(张萌)1, Shengnan Dai(戴胜男)2,†, Ranran Zhang(张冉冉)3, Mingfang Shu(舒明方)1, Wei Xu(徐威)1, Jinfeng Zhu(朱金峰)1, Xianglin Liu(刘祥麟)4, Yixuan Luo(罗伊轩)4, Toru Ishigaki5, Bo Duan(段波)6, Yanfeng Guo(郭艳峰)4,7, Zhe Qu(屈哲)3, Jiong Yang(杨炯)2, and Jie Ma(马杰)1,‡   

  1. 1 Key Laboratory of Artificial Structures and Quantum Control, School of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai 200240, China;
    2 Materials Genome Institute, Shanghai University, Shanghai 200444, China;
    3 Anhui Key Laboratory of Low-Energy Quantum Materials and Devices, High Magnetic Field Laboratory, Hefei Institutes of Physical Science, Chinese Academy of Sciences, Hefei 230031, China;
    4 School of Physical Science and Technology, ShanghaiTech University, Shanghai 201210, China;
    5 Neutron Industrial Application Promotion Center, Comprehensive Research Organization for Science and Society, Naka, Ibaraki 319-1106, Japan;
    6 Hubei Key Laboratory of Theory and Application of Advanced Materials Mechanics, School of Science, Wuhan University of Technology, Wuhan 430070, China;
    7 ShanghaiTech Laboratory for Topological Physics, ShanghaiTech University, Shanghai 201210, China
  • Received:2025-04-05 Revised:2025-05-06 Accepted:2025-05-19 Online:2025-07-17 Published:2025-08-05
  • Contact: Shengnan Dai, Jie Ma E-mail:musenc@shu.edu.cn;jma3@sjtu.edu.cn
  • Supported by:
    Project supported by the National Natural Science Foundation of China (Grant Nos. U2032213 and 12334008), the Guangdong Provincial Key Laboratory of Extreme Conditions (Grant No. 2023B1212010002). We thank the staff members of the Micro-Raman Spectroscopy System (https://cstr.cn/31125.02.SHMFF.RAMAN) at the Steady High Magnetic Field Facility, CAS (https://cstr.cn/31125.02.SHMFF), for providing technical support and assistance in data collection and analysis. We acknowledge the beam time granted by J-PARC (proposal No. 2019A0191).

摘要: The family of transition-metal dipnictides, $MX_{2}$ ($M$: metal, $X$: N, P, As, Sb, and Bi), has emerged as an important quantum material system due to its unique physical properties, such as large magnetoresistance, colossal Seebeck coefficients, and Weyl semimetal characteristics. In order to study the $M$-site ions effect on the lattice structure and the related dynamics, we compared two isostructural compounds, FeSb$_{2}$ and RuSb$_{2}$. Neutron diffraction, specific heat, and Raman scattering spectra of RuSb$_{2}$ were measured. We found that the thermal expansion coefficients are isotropic for RuSb$_{2}$, in contrast to the anisotropic behavior reported previously in FeSb$_{2}$. Moreover, the specific heat of RuSb$_{2}$ shows a boson-like anomaly around 25 K. Four of the six predicted vibrational modes were identified by polarized Raman scattering spectra and successfully simulated by ab initio calculations. Meanwhile, the temperature-dependent linewidths reveal that phonon-phonon interactions might dominate above 50 K, while electron-phonon coupling remains relatively weak.

关键词: transition-metal dipnictide, neutron diffraction, Raman, boson-like peak

Abstract: The family of transition-metal dipnictides, $MX_{2}$ ($M$: metal, $X$: N, P, As, Sb, and Bi), has emerged as an important quantum material system due to its unique physical properties, such as large magnetoresistance, colossal Seebeck coefficients, and Weyl semimetal characteristics. In order to study the $M$-site ions effect on the lattice structure and the related dynamics, we compared two isostructural compounds, FeSb$_{2}$ and RuSb$_{2}$. Neutron diffraction, specific heat, and Raman scattering spectra of RuSb$_{2}$ were measured. We found that the thermal expansion coefficients are isotropic for RuSb$_{2}$, in contrast to the anisotropic behavior reported previously in FeSb$_{2}$. Moreover, the specific heat of RuSb$_{2}$ shows a boson-like anomaly around 25 K. Four of the six predicted vibrational modes were identified by polarized Raman scattering spectra and successfully simulated by ab initio calculations. Meanwhile, the temperature-dependent linewidths reveal that phonon-phonon interactions might dominate above 50 K, while electron-phonon coupling remains relatively weak.

Key words: transition-metal dipnictide, neutron diffraction, Raman, boson-like peak

中图分类号:  (Phonons in crystal lattices)

  • 63.20.-e
61.05.F- (Neutron diffraction and scattering) 63.20.Ry (Anharmonic lattice modes) 78.30.-j (Infrared and Raman spectra)